Fluid Dynamics and Its Biological and Medical Applications
Fluid Dynamics and Its Biological and Medical Applications
91 Molecular Transport Phenomena: Diffusion, Osmosis, and Related Processes
Learning Objectives
- Define diffusion, osmosis, dialysis, and active transport.
- Calculate diffusion rates.
Diffusion
There is something fishy about the ice cube from your freezer—how did it pick up those food odors? How does soaking a sprained ankle in Epsom salt reduce swelling? The answer to these questions are related to atomic and molecular transport phenomena—another mode of fluid motion. Atoms and molecules are in constant motion at any temperature. In fluids they move about randomly even in the absence of macroscopic flow. This motion is called a random walk and is illustrated in Figure 91.1 . Diffusion is the movement of substances due to random thermal molecular motion. Fluids, like fish fumes or odors entering ice cubes, can even diffuse through solids.
Diffusion is a slow process over macroscopic distances. The densities of common materials are great enough that molecules cannot travel very far before having a collision that can scatter them in any direction, including straight backward. It can be shown that the average distance [latex]{x}_{\text{rms}}[/latex] that a molecule travels is proportional to the square root of time:
where [latex]{x}_{\text{rms}}[/latex] stands for the root-mean-square distance and is the statistical average for the process. The quantity [latex]D[/latex] is the diffusion constant for the particular molecule in a specific medium. Table 91.1 lists representative values of [latex]D[/latex] for various substances, in units of [latex]{\text{m}}^{2}\text{/s}[/latex].
| Diffusing molecule | Medium | D (m2/s) |
|---|---|---|
| Hydrogen [latex]\left({\text{H}}_{2}\right)[/latex] | Air | [latex]6.4×{10}^{–5}[/latex] |
| Oxygen [latex]\left({\text{O}}_{2}\right)[/latex] | Air | [latex]1.8×{10}^{–5}[/latex] |
| Oxygen [latex]\left({\text{O}}_{2}\right)[/latex] | Water | [latex]1.0×{10}^{–9}[/latex] |
| Glucose [latex]\left({\text{C}}_{6}{\text{H}}_{12}{\text{O}}_{6}\right)[/latex] | Water | [latex]6.7×{10}^{–10}[/latex] |
| Hemoglobin | Water | [latex]6.9×{10}^{–11}[/latex] |
| DNA | Water | [latex]1.3×{10}^{–12}[/latex] |
Note that [latex]D[/latex] gets progressively smaller for more massive molecules. This decrease is because the average molecular speed at a given temperature is inversely proportional to molecular mass. Thus the more massive molecules diffuse more slowly. Another interesting point is that [latex]D[/latex] for oxygen in air is much greater than [latex]D[/latex] for oxygen in water. In water, an oxygen molecule makes many more collisions in its random walk and is slowed considerably. In water, an oxygen molecule moves only about [latex]40\phantom{\rule{0.25em}{0ex}}\mu \text{m}[/latex] in 1 s. (Each molecule actually collides about [latex]{\text{10}}^{\text{10}}[/latex] times per second!). Finally, note that diffusion constants increase with temperature, because averag